Thermoelectric electrochemical conversion devices

ABSTRACT

A heat capacitor with simple structure, easy to manufacture and high thermoelectric conversion efficiency is provided. The heat capacitor includes: a pair of electrodes, at least one said electrode being a carbonaceous electrode; and a thermoelectric electrolyte disposed between the pair of electrodes, wherein the distance between the pair of electrodes is at most 1 mm.

CROSS REFERENCE TO RELATED APPLICATIONS

The present application claims priority to U.S. provisional ApplicationNo. 62/874,488, filed on Jul. 15, 2019, which is incorporated herein byreference in its entirety for all purposes.

FIELD OF THE INVENTION

The present disclosure relates to a thermoelectric conversion deviceand, more particularly, to a heat capacitor with simple structure, easyto manufacture and high thermoelectric conversion efficiency.

BACKGROUND OF THE INVENTION

Thermoelectric (TE) devices are electronic devices for convertingtemperature differences into electrical energy and vice versa. Aresearch topic which is increasingly becoming popular is the potentialapplication of thermoelectric devices to power generation andtemperature control. A common example of thermoelectric devices is athermoelectric cooler (TEC) or thermoelectric generator (TEG) whichoperates by coupling and transmission between electrons and phonons.

Important characteristics of thermoelectric materials includethermoelectric figure-of-merit (ZT) which is directly related to theconversion efficiency of the thermoelectric devices. For athermoelectric material to be high-efficiency, it must have high thermaldiffusivity but low thermal conductivity. From the perspective ofindustrial application, the conventional ways of power generation can bethoroughly changed, if a thermoelectric device of ZT level higher than1.4 is developed.

Conventional thermoelectric devices are mostly solid-state semiconductordevices, with p-type and n-type semiconductor pins connected byelectrical series connection and thermal parallel connection. However,the solid materials for use as p-type and n-type semiconductorsaccording to the prior art have a disadvantageous physical property,i.e., low conversion efficiency, to the detriment of their industrialapplication.

The prior art also discloses combining nano-printed thermoelectricmaterials and doping semiconductors, such that they have anelectron-rich state or electron-depleted state and thereby satisfactorythermoelectric conversion efficiency. However, both the aforesaid twotechniques have their own intractable drawbacks.

One of the advantages of nano-printed semiconductor structure lies inthe promising nano-printing technology. However, with printing arearequirement on the rise, properties of semiconductor structure areincreasingly difficult to control. Doping mechanism still relies onexpensive doping elements and harmful doping techniques to the detrimentof its wide application.

The aforesaid drawbacks of solid-state thermoelectric semiconductordevices inspire researchers to study thermoelectric properties ofpolymeric electrolytes. For instance, US 2013/0276850 A1 discloses athermoelectric device capable of converting a temperature differenceinto electrical energy according to two different electrolyteproperties. The thermoelectric device is structurally complicated andrequires a connector and at least one pin to transmit ions. Furthermore,the thermoelectric device not only requires a solid-state electrolytesoluble in water and dissociated therein but also requires a conductivepolymer for electrical transmission of ions. In short, thethermoelectric device requires plenty, different constituent componentsto collect thermoelectric energy and charges its capacitors with theelectrical power.

In Zhao, D., Wang, H., Ullah Khan, Z., Chen, J. C., Gabrielsson, R.,Jonsson, M., Berggren, M., Crispin, X., (2016). Ionic thermoelectricsupercapacitors. Energy & Environmental Science, 9 (4), 1450-1457, Zhao,D., Wang and others disclose that temperature gradient can be convertedinto molecular concentration gradient in a solution through thermaldiffusivity effect (Soret effect) and causes a thermoelectric voltage.The thermoelectric voltage is determined according to ionic Seebeckcoefficient α_(i) and thermal gradient ΔT across the electrolyte. Thusfar, ionic thermoelectric supercapacitor (ITESC) has converted thermalenergy into stored electric charges by ionic Soret effect, therebyproviding a new way to collect energy from an intermittent heat source.Compared with a conventional thermoelectric generator, ITESC can convertand store more energy.

SUMMARY OF THE INVENTION

Conventional heat capacitors are structurally complicated to thedetriment of ease of manufacturing and cost effectiveness. In order toovercome the aforesaid drawbacks of the prior art, it is an objective ofthe present disclosure to provide a heat capacitor which is structurallysimple, easy to manufacture, and has high thermoelectric conversionefficiency with a view to achieving high-efficiency manufacturing, lowcost and an alternative green energy source.

An aspect of the present disclosure provides a heat capacitor,comprising: a pair of electrodes, at least one said electrode being acarbonaceous electrode; and a thermoelectric electrolyte disposedbetween the pair of electrodes, wherein the distance between the pair ofelectrodes is at most 1 mm.

According to an embodiment of the present disclosure, the carbonaceouselectrode is made of graphene, carbon nanotubes, nano-, micro- ormeso-porous pure carbon film, composite carbon film, or a combinationthereof.

Considering the space between the pair of electrodes is very limited, itis difficult to place a thermoelectric electrolyte in the space. In anembodiment, the thermoelectric electrolyte is fluid or semifluid and isdisposed between the pair of electrodes by being injected with a tinyneedle or injector.

In yet another embodiment, the thermoelectric electrolyte is film.Optionally, the thermoelectric electrolyte is gel-like electrolyte. Thegel-like electrolyte is absorbed by and anchored to a porous membrane.Then, the porous membrane is inserted into between the pair ofelectrodes. Alternatively, an electrode, a membrane which theelectrolyte is absorbed by and anchored to, and another electrode aresequentially stacked up to form a heat capacitor.

According to another embodiment of the present disclosure, the heatcapacitor further comprises a non-conductive package member surroundingand protecting the thermoelectric electrolyte, but this technicalfeature is not an essential technical feature of the present disclosure.

Regarding the other aspects of the present disclosure, some aredescribed later, whereas some other can be inferred easily from thedescription or inferred from the implementation of the presentdisclosure. Every aspect of the present disclosure can be comprehendedand accomplished by way of components specified in the appended claimsand combinations thereof. Both the foregoing general description and thedetailed description below are illustrative, rather than restrictive, ofthe present disclosure.

BRIEF DESCRIPTION OF THE DRAWINGS

The present disclosure is hereunder illustrated with embodiments inconjunction with the accompanying drawings, in which:

FIG. 1 is a cross-sectional view of a heat capacitor according to anembodiment of the present disclosure.

FIG. 2A and FIG. 2B are schematic views of how to form impregnatedgel-like electrolyte according to an embodiment of the presentdisclosure.

FIG. 3 is a cross-sectional view of the heat capacitor with a packagemember according to an embodiment of the present disclosure.

FIG. 4A is a voltage versus temperature difference graph of the heatcapacitor according to an embodiment of the present disclosure.

FIG. 4B is an actual temperature versus temperature difference graph ofthe heat capacitor according to an embodiment of the present disclosure.

FIG. 5 is cyclic voltammogram of the heat capacitor according to anembodiment of the present disclosure.

FIG. 6A and FIG. 6B are graphs of rapid kinetics of electric chargeaccumulation of the heat capacitor according to an embodiment of thepresent disclosure.

FIG. 7A through FIG. 7C are energy-voltage graph, current-voltage graph,and maximum power—voltage graph of the heat capacitor according to anembodiment of the present disclosure, respectively.

FIG. 8 is a graph of behavior of the heat capacitor after removal of aheat source according to an embodiment of the present disclosure.

DETAILED DESCRIPTION OF THE INVENTION

The present disclosure provides a heat capacitor with simple structure,easy to manufacture and high thermoelectric conversion efficiency with aview to achieving high-efficiency manufacturing, low cost and analternative green energy source. The present disclosure is depicted withaccompanying drawings and described below. In the accompanying drawings,like reference numerals denote like components. Devices, components andprocess steps in the embodiments described below are illustrative of thepresent disclosure rather than restrictive of the scope of the presentdisclosure.

Researchers had applied a low power solution, such as piezoelectriceffect and magnetoelectric effect, to aid the power generation ofthermoelectric devices. According to fundamental principles related tothermal energy and comprehensible to persons skilled in the art,temperature represents average energy of molecules and particles withina volume or region and corresponds to particles and molecules ofdifferent mass moving at different velocity, such that energy of theentire system is at equilibrium, where the average temperature isdenoted by T.E=m·c ²  (1)

Formula (1) expresses mass-energy equivalence proposed by AlbertEinstein, suggesting that energy is intrinsically work, wherein work isthe product of force and distance, and force is the product of mass andacceleration. For the sake of illustration, distance is set to onemeter, time to one second, and energy to one watt. Formula (1) isconverted into formula (2) below.E=Q=1 watt=m·a  (2)

Referring to formula (2), when two particles or molecules of differentmass receive the same amount of energy, the lighter particle or moleculemoves with a greater acceleration and to a greater distance. Therefore,particles or molecules of low mass have high diffusivity rate.

The analysis below is based on the assumption that a heat capacitor hassmall particles/molecules carrying positive electric charges and largeparticles/molecules carrying negative electric charges. If the top ofthe heat capacitor is heated up, the heat capacitor will have atemperature difference in its entirety, the small particles carryingpositive electric charges will move quickly and thus diffuse to thebottom surface to form a uniform layer, but most large moleculescarrying negative electric charges will stay and stack up on the top. Asa result, the bottom and top surfaces generate electrostatic charges byinduction in the presence of particles carrying positive and negativeelectric charges, respectively. The aforesaid process is performedrepeatedly until the positive and negative electric charges stack up andaccumulate on the top and bottom surfaces. Therefore, a bilayercapacitor with sufficient electric charges is formed.

If diffusion length of cations (i.e., the distance traveled by cationsto the negative electrode in the heat capacitor) is reduced, electriccharge accumulation speed will increase. The increase in the electriccharge accumulation speed is conducive to timely, effective creation ofinternal electric field and separation of electric charges (cations andanions). When one of the two electrodes is heated up, cations (i.e.,mobile ions) diffuse out of the heated electrode to thereby move awaytherefrom and adsorb large anions within a negative potential range. Asthe reduction in the diffusion length continues, some cations take lesstime to reach the cold electrode, thereby creating internal electricfield between the two electrodes. However, at this point in time, theelectric field between the two electrodes is not at equilibrium andrequires redistribution of electric charges in order for the electricfield to be at equilibrium. Upon the redistribution of electric charges,a bilayer structure is formed in both the two electrodes, and the heatcapacitor is charged. The reduction in the distance between theelectrodes causes a reduction in the temperature difference required forcompletely charging a thermoelectric apparatus. Thus, the technicalfeatures in an embodiment of the present disclosure are applicable to aheat capacitor conducive to achievement of Seebeck/Soret effect greaterthan 100 my/K. Furthermore, a reduction in the distance betweenelectrodes, whatever the type of the electrodes, enhances the efficiencyof converting thermal energy into electrical energy. This kind ofsynergy also occurs to electrolyte redox couple, ferrocyanide andferricyanide.

FIG. 1 is a cross-sectional view of a heat capacitor according to anembodiment of the present disclosure. The heat capacitor 10 comprises: apair of electrodes 12, 16, at least one of which is a carbonaceouselectrode; and a thermoelectric electrolyte 14 disposed between the pairof electrodes 12, 16, wherein the distance between the pair ofelectrodes is at most 1 mm.

For the sake of illustration, the present disclosure provides a specificembodiment intended to illustrate the feasibility of the embodiment ofFIG. 1 rather than limit the claims of the present disclosure. First, apair of glass substrates disposed opposite to each other are provided.Preferably, the pair of glass substrates are parallel. After that,conductive carbon paste is coated on opposite surfaces of the pair ofglass substrates, respectively, to function as a pair of electrodes 12,16 of the heat capacitor 10. Next, a seal layer is formed at theperiphery of the glass substrates and fixes the distance between theopposing substrates, such that a space is formed between the electrodes12, 16. The distance between the electrodes 12, 16 is at most 1 mm, atmost 0.9 mm, or at most 0.8 mm. Finally, the thermoelectric electrolyte14, which is fluid, is injected into the space between the opposingsubstrates (i.e., the pair of electrodes 12, 16) with an injector toform the heat capacitor 10.

The heat capacitor 10 will work, provided that one of the electrodes 12,16 is made of carbonaceous materials; however, the electrodes 12, 16described above merely serve an exemplary purpose and thus are notrestrictive of the present disclosure. The carbonaceous materialsinclude all materials related to carbon, including carbon-likematerials, carbon-containing materials, and pseudo-carbon materials.

In an embodiment of the present disclosure, the carbonaceous electrodecomprises, but is not limited to, graphene, carbon nanotubes, nano-,micro- or meso-porous composite carbon film or pure carbon film. Themeso-materials disclosed herein must be interpreted to include mostcarbon materials. Not all the electrodes are necessarily made of purecarbon materials; instead, the electrodes may be made ofcarbon-containing composite.

Although metallic electrodes are provided in an embodiment of thepresent disclosure, the metallic electrodes are less satisfactory thancarbonaceous electrodes. In an embodiment of the present disclosure, themajor advantage of carbonaceous electrodes (for example, activatedcarbon) lies in porosity of carbon particles. When carbon particles areactivated, their porosity and high surface area enable them to adsorbmore ions and thus accumulate or store more electric charges, so as tobe prepared to discharge.

In an embodiment of the present disclosure, the structure and porosityof carbonaceous electrodes is described in terms of nano-, micro- ormeso-porosity with a view to defining the corresponding heat capacitorstructure. For example, nano-porous carbon electrodes are made of carbonand have nanoscale tunnels and pores to increase the specific area ofthe electrodes and thus enhance the performance of electrolytes. Theexpression “meso-” refers to any dimensions greater than “micro-”, forexample, millimeter, a unit of length.

In an embodiment of the present disclosure, carbonaceous compositeelectrodes are doped with a transition metal oxide (for example, MnO₂).The transition metal oxide disclosed herein is illustrative, rather thanrestrictive, of the present disclosure. Preferably, in an embodiment ofthe present disclosure, the electrodes can be covered with graphene,graphene oxide, carbon nanotubes, activated carbon, glass carbon,graphite or a combination thereof.

FIG. 2A and FIG. 2B are schematic views of how to form impregnatedgel-like electrolyte according to an embodiment of the presentdisclosure. For example, a membrane 14 a is impregnated with gel-likeelectrolyte, such that the electrolyte is absorbed by and anchored tothe membrane 14 a. In an embodiment, the membrane 14 a is a porouscellulose membrane (model number: TF4035) developed by NKK. The gel-likeelectrolyte is absorbed by and anchored to the cellulose membrane. Then,a gel-like electrolyte-containing membrane 14 b is inserted into betweenthe electrodes 12, 16. The NKK-developed TF4035 membrane not onlyabsorbs and anchors the electrolyte but also separates the electrodes toprevent the electrodes from coming into direct contact with each other,thereby functioning as a baffle for use in a conventional battery,capacitor or fuel battery.

In an embodiment, the membrane 14 a can be dispensed with, but the useof a membrane can make the entire manufacturing process simple if theelectrolyte is gel (highly viscous liquid). The purpose of the membraneis to absorb and anchor gel-like electrolyte. Therefore, the gel-likeelectrolyte-containing membrane 14 b is directly inserted into betweenthe electrodes 12, 16 to dispense with the step of forming a seal layerand injecting electrolyte.

The membrane and the electrolyte are different. The purpose of themembrane is to absorb and anchor electrolyte and separate theelectrodes. The membrane advantageously reduces the manufacturing costsand simplifies the manufacturing process.

Water is regarded as an impurity to the electrolyte in an embodiment ofthe present disclosure. By contrast, the electrolyte in thethermoelectric system of another embodiment of the present disclosurecontains a small amount of water. The electrolyte contains, but is notlimited to, polyethylene glycol (PEG). The electrolyte is, but is notlimited to, molten salt which comprises potassium hydroxide and rubidiumhydroxide, including, but not limited to, PEG-LiOH, PEG-NaOH, PEG-KOH,PEG-RbOH, and PEG-CsOH.

In an embodiment of the present disclosure, electrolyte is, for example,low-molecular-weight PEG to form molten salt (alkali salt reacts withPEG to form molten salt) and undergo dehydration. In an alternativeembodiment, for example, electrolyte is an aqueous solution offerrous/ferrocyanide redox couple, an aqueous solution of iodide/iodineredox couple, or organic/inorganic salts soluble in a specific solvent.In the alternative embodiment, the electrolyte can be formed, providedthat the salts are mixed and fixed together, such that cations andanions in the system, for example, water or dimethylformamide (DMF),wherein DMF is a common organic solvent for use in an energy storagesystem (such as a battery). In short, a specific amount of potassiumhydroxide and PEG are mixed therein and heated up at a specifictemperature and within a time period to enable a reaction therebetween,thereby attaining a suitable electrolyte. A trace of water remains inthe electrolyte, regardless of how much water is removed.

FIG. 3 is a cross-sectional view of the heat capacitor with a packagemember according to an embodiment of the present disclosure. Referringto FIG. 3, the heat capacitor 10 further comprises a non-conductivepackage member 18 surrounding and protecting the thermoelectricelectrolyte. The package member 18 comprises a polymer, for example,acrylonitrile-butadiene-styrene (ABS) or polydimethylsiloxane (PDMS),but is not limited thereto.

The package member 18 can be made of any materials, provided that it isnon-conductive and unlikely to cause the electrodes to short-circuit.Examples of the materials include rubber, plastic, polymeric aluminum,and ceramic, depending on the manufacturing process. For example,plastic like polyethene is not suitable for a high-temperature operationenvironment. Soft materials, such as plastic and homogeneous materials,are suitable for contact with the human skin.

An embodiment of the present disclosure provides a heat capacitordevice. The heat capacitor device is a heat capacitor (G0.1 battery forshort) formed by, for example, mounting a commercially-available carbonfabric and activated carbon on a copper substrate. The copper substratefunctions as a current collector (collector for short) which is a thinmetal plate attached to the electrodes to collect electric current fromthe battery fully. The carbonaceous electrodes are usually deposited onthe copper foil to effect electrical contact. In this embodiment, evenif the battery dispenses with a collector, the battery will worksmoothly. Afterward, the NKK-developed TF4035 cellulose membrane fixesthe distance between the electrodes, and PEG-KOH serves as thethermoelectric electrolyte, with a K-type thermoelectric couple adaptedto measure and record temperature. During a test, the heat capacitordevice is attached to a hot water bottle.

FIG. 4A is a voltage versus temperature difference graph of the heatcapacitor according to an embodiment of the present disclosure.

FIG. 4B is an actual temperature versus temperature difference graph ofthe heat capacitor according to an embodiment of the present disclosure.

For the sake of comparison with conventional data, the data of G0.1battery is herein provided, such that G0.1 battery attains a capacitanceof 1 μF. FIG. 5 is cyclic voltammogram of the heat capacitor accordingto an embodiment of the present disclosure.

In the embodiment illustrated by FIG. 5, the cyclic voltammogram of G0.1battery is almost in rectangular shape, confirming the absence ofbilayer capacitor mechanism of any chemical reaction.

In an embodiment of the present disclosure, G0.1 battery is astructurally-simple, symmetrical battery and comprises unprocessed,commercially-available carbon fabric whose area is, for example, 4×5cm², to function as a pair of electrodes in the presence of PEG-KOHelectrolyte. FIG. 6A and FIG. 6B are graphs of rapid kinetics ofelectric charge accumulation of the heat capacitor according to anembodiment of the present disclosure. In the course of transientdischarging, electric charges of the heat capacitor accumulate, anew andfaster, at the fourth minute when compared to the first-instancecharging. The foregoing result also confirms that this embodiment of thepresent disclosure does not require a thermodynamic cycle to regeneratedand reactivate a battery.

FIG. 7A through FIG. 7C are energy-voltage graph, current-voltage graph,and maximum power—voltage graph of the heat capacitor according to anembodiment of the present disclosure, respectively. FIG. 7A through FIG.7C show the specific levels of power and energy of the heat capacitorwhen rated capacitance of the heat capacitor is around 1 μF.

Another important technical feature of the present disclosure is theelectric charge retention rate after removal of heat.

FIG. 8 is a graph of behavior of the heat capacitor after removal of aheat source according to an embodiment of the present disclosure.Although the heat capacitor discharges spontaneously at the 16th minute,electric charges accumulate spontaneously to attain a higher voltage aswell, thereby dispensing with any additional heat sources.

Assuming that capacitance has nothing to do with temperature, i.e.,Q=CV. (Table 1 shows an estimation made visually.)

TABLE 1 G0.1 battery G0.1 (discharging battery which follows (instantequilibrium in discharging) 600 seconds) Q_(charging) (C) 1 μC   1 μCQ_(discharging) (C) 1 μC 1.5 μC Q_(discharging)/Q_(charging) (%) 100%150%

In this embodiment, the electrolyte of the heat capacitor is not onlynon-volatile and non-toxic but also extremely stable at roomtemperature. Generation of current from a heat capacitor can be achievedby the use of cheap electrodes rather than expensive electrodes made ofprecious metals, for example, gold.

As regards the heat capacitor of the present disclosure, electrodesurface area is an important factor. The electrodes are made ofnano-scale or micro-scale carbon materials, for example, carbonnanotubes and activated carbon with high surface area. In anotherembodiment of the present disclosure, carbon fabric functions aselectrodes.

Given the formula, C=Q/V=εA/d, the capacitance of the battery depends onthe area of electrodes and the distance between the electrodes, which inturn depend on the voltage and the amount of electric charges generatedby each battery. However, these are only some of the factors inparameters, such as electric charge storage.

Electrochemical activated surface area (EASA) is another factor inelectric charge storage. When some activated materials (for example,MnO₂) are deposited on electrodes (such as carbon fabric), their EASAallows admission of electrolyte to attain electric charge transferand/or storage.

In an embodiment of the present disclosure, the heat capacitor comprisesor does not comprise a membrane between two electrodes. The membrane isfunctionalized and shortens the distance between the electrodes.Intrinsically, the membrane merely functions as a short-distance elementbetween the electrodes. Most importantly, the electrolyte transfers ionsin a direction perpendicular to the electrodes. The electrolytecomprises, but is not limited to, alkali metal-containing molten saltwhich contains large counter-anions. In an embodiment of the presentdisclosure, the electrolyte is preferably chlorine-free. It is because,in the course of operation of the battery, chlorides tend to producechlorine gas which is harmful to the human body and environment. Thethickness of the electrode sandwich structure is less than 1 mm. In anembodiment of the present disclosure, the heat capacitor functions as asupercapacitor independently and operates together with a hot waterbottle to collect electrical energy generated from the heat capacitor.

In an embodiment of the present disclosure, the heat capacitor deviceprovided is characterized in that the distance between the electrodes isnot greater than 1 mm. The diffusive length of cations is shortened, andthe time required for the built up of electric double layer is reduced.In principle, it is preferable to achieve higher capacitance with moreelectric charges, the compact designs such as making series connectionexpand to the stacked battery, and new battery settles. At least one ofthe electrodes is made of highly conductive pseudo-carbon materials toincrease the specific area of the electrodes and increase the contactarea of the electrolyte. The capacitance retention rate is high,indicating that the heat capacitor maintains most of its performancewith minimum reduction thereof even after going through thousands ofcycles.

An embodiment of the present disclosure provides a membrane which iseasy to manufacture and incurs low cost, especially when the electrolyteis not solid-state. The distance between the electrodes (for example,but is not limited to, 35 μm) is easily adjusted by producing or usingmembranes of different thickness. In particular, owing to the use of themolten salt electrolyte (for example, PEG-KOH), interaction of thermalenergy is restricted to allowing only small cations to form largepolymeric chain-structured anions and avoiding the use of harmfulsolvent and organic salt. Like a conventional battery, high viscosity isassociated with low chance of leakage of electrolyte out of the system.

Although the present disclosure is disclosed above by variousembodiments, the embodiments are not restrictive of the scope of thepresent disclosure. Changes and modifications made by persons skilled inthe art to the embodiments without departing from the spirit and scopeof the present disclosure must be deemed falling within the scope of thepresent disclosure. Accordingly, the legal protection for the presentdisclosure should be defined by the appended claims.

What is claimed is:
 1. A thermoelectric electrochemical conversiondevice, comprising: a pair of electrodes configured to be applied with atemperature differential, at least one said electrode being acarbonaceous electrode; and a polymeric thermoelectric electrolytedisposed between the pair of electrodes, such that the appliedtemperature differential over said pair of electrodes makes mobile ionsdiffuse via the thermoelectric electrolyte towards a lower temperatureelectrode of the pair of electrodes in accordance with a Seebeck/Soreteffect and generate a thermoelectric voltage, wherein a distance betweenthe pair of electrodes is at most 1 mm.
 2. The thermoelectricelectrochemical conversion device of claim 1, wherein the carbonaceouselectrode comprises graphene, carbon nanotubes, nano-, micro- or meso-porous pure carbon film, composite carbon film, or a combinationthereof.
 3. The thermoelectric electrochemical conversion device ofclaim 1, wherein the polymeric thermoelectric electrolyte is fluid orsemifluid and is disposed between the pair of electrodes by injection.4. The thermoelectric electrochemical conversion device of claim 1,wherein the polymeric thermoelectric electrolyte is gel.
 5. Thethermoelectric electrochemical conversion device of claim 4, furthercomprising a membrane disposed between the pair of electrodes, with thepolymeric thermoelectric electrolyte absorbed by and anchored to themembrane.
 6. The thermoelectric electrochemical conversion device ofclaim 1, wherein the polymeric thermoelectric electrolyte comprisesanhydrous molten salt.
 7. The thermoelectric electrochemical conversiondevice of claim 1, wherein the polymeric thermoelectric electrolytecomprises an alkali metal with large anions.
 8. The thermoelectricelectrochemical conversion device of claim 1, further comprising anon-conductive package member surrounding and protecting the polymericthermoelectric electrolyte.
 9. The thermoelectric electrochemicalconversion device of claim 1, wherein the package member comprises apolymer.
 10. The thermoelectric electrochemical conversion device ofclaim 9, wherein the polymer comprises ABS or PDMS.